EP2024447B1

EP2024447B1 - Matrix comprising zero-order diffractive pigments

Info

Publication number: EP2024447B1
Application number: EP07701926A
Authority: EP
Inventors: Harald Walter; Alexander Stuck
Original assignee: Centre Suisse dElectronique et Microtechnique SA CSEM
Current assignee: Centre Suisse dElectronique et Microtechnique SA CSEM
Priority date: 2006-05-31
Filing date: 2007-03-08
Publication date: 2011-06-29
Anticipated expiration: 2027-03-08
Also published as: EP2024447A1; US7974010B2; WO2007137438A1; JP2009538937A; PL2024447T3; US20090257126A1; ATE514756T1

Abstract

The present invention relates to pigments comprising or consisting of a layer made of a material with an index of refraction that is higher than the index of refraction of the adjacent material by at least 0.25; whereas said layer has a zero-order diffractive micro-structure; whereas said layer acts as an optical waveguide and whereas said layer has a thickness between 50 nm and 500 nm; to processes for its manufacture and to its use. These pigments show a color effect upon rotation and/or tilting, and it is believed that this color effect is based on zero-order diffraction.

Description

The present invention relates to pigments showing a colour effect upon rotation and/or tilting, in particular to colour effect pigments wherein the colour effect is based on zero-order diffraction, to processes for its manufacture and to its use.
Physical colour: It is known to obtain physical colour either by first and higher order diffraction of a surface grating or by flat dielectric layer stacks or Fabry-Perot type layer stacks (interference filters) which are disclosed in US3858977 . It is also known that physical colours can be obtained by combining very fine, subwavelength gratings, with one or several dielectric and/or metal stacks on it. Such so called zero order diffractive filter (ZOD filter) or zero order diffractive device (ZOD device) uses zero order diffraction to produce very pronounced colour effects as described in US4484797 . Main features and advantages of ZOD devices are:

Iridescent optical effect, which varies with tilting angle Θ and/or rotation angle φ
optical effect is easily recognized by untrained people
optical effect is machine readable
Strong colour effect, even under diffuse lighting conditions
Cost effective, mass producible technique are available
Very difficult to counterfeit, as the optical effect depends on the material properties, the deposition of high index material on 2 different levels combined with an extremely fine, sub-wavelength grating. Copying only the grating or the material stack will not produce the desired effect.

ZOD devices: As is shown in fig. 1.1, a typical ZOD structure consists of a low index of refraction (LRI) material (white, n₁ in the range of 1.1-1.7) in which segments of a material (HRI layer) with a higher index of refraction (black, n₂>n₁+0.25) are regularly arranged on a periodic microstructure, e.g. parallel or crossed grating lines. More general either the waveguiding layer is modulated with the diffractive microstructures or the microstructures are placed on top or below this layer. The material above and below the waveguide can have a different index of refraction. One can even be air. In order for zero order diffraction to take place a number of parameters have to be adjusted including microstructure period A, microstructure depth t, thickness of the waveguiding layer c, the fill factor or duty cycle f.f.=p/Λ and the microstructure profile or shape (rectangular, sinusoidal, triangular or more complex). The period of the microstructures is smaller than the wavelength of light for which the filter is designed. If illuminated by white light, this ZOD structure directly reflects a particular spectral range or colour very efficiently. This comes from a resonance effect in the subwavelength grating structured wave-guiding HRI layer. This layer acts as a leaky waveguide. Therefore ZOD filters are sometimes called resonant gratings. A part of the light incident at an angle Θ is directly transmitted and a part is diffracted and trapped in the waveguiding layer. Some of the trapped light is rediffracted out and interferes with the transmitted part. At a certain wavelength and angular orientation φ of the periodic microstructure a resonance occurs which leads to complete destructive interference. No such light is transmitted. Contrary to first or higher order diffraction devices, in ZOD devices or ZOD filters the light is reflected at a viewing angle which is equal to the incidence angle Θ. As long as the materials used possess no absorption the transmission spectra are the complement of those in reflection. More details concerning zero-order diffractive filters can be found in M.T. Gale, "Zero-Order Grating Microstructures" in R.L. van Renesse, Optical Document Security, 2nd Ed., pp. 267-287. The reflected and transmitted colour depends on the orientation of the grating with respect to the observer. As is indicated in fig. 1.2, the colour changes upon rotation about the surface normal ("colour flip"). Depending on the symmetry of the grating, different rotation angles can be achieved. In linear gratings, the spectra are identical, if the ZOD grating is rotated by 180°, but a strong colour flip occurs upon 90° rotation. In 2-dimensional gratings, 60° and 90° symmetric colour flip effects can be easily made, other values are also possible. Reflectivity of 100% at specific wavelengths is theoretically possible; in practice values up to 80-90% are observed.
Manufacturing of ZOD filters: It is known to manufacture ZOD filters as laminated foils in roll to roll processes with thermally evaporated ZnS as the HRI layer deposited on foil substrates which were micro-structured by hot-embossing.
Use of ZOD filters: It is known to use the foils manufactured as described above as security features for passport and document protection, as well as in banknotes. ZOD filters are considered a natural successor of the now widely used holograms for security applications. A main reason is that ZOD filters are more difficult to counterfeit, yet use the same basic production technologies, as holograms. Further, ZOD filters are better visible for the human eye and can be easily checked with simple machines.
Colour shifting pigments: It is also known that colour shifting pigments can be manufactured by multilayer deposition of alternating high and low index of refraction layers or a Fabry-Perot type interference layer stack. The colour shifting comes from thin film interference effects in the multilayer stacks.
US5135812 describes processes for manufacturing such pigments based on vacuum deposition. On one surface of a flexible web of material an optically variable thin film coating is formed. The coating is separated from the web to form optically variable thin film flakes. The flakes are disposed in ink and paint vehicles to provide optically variable inks. It is considered disadvantageous that the thus obtained pigments do not show a pronounced colour effect upon rotation. Furthermore at least five layer must be deposited which is rather costly and leads to thick pigments. Typically such pigments are on the order of 1µm thick.
WO98/53012A1 describes alternative methods to manufacture pigments with such multilayer stacks based on deposition of the layers from gas or liquid phases. Multi-coated interference pigments which are obtained by hardening and by hydrolysis of an aqueous solution of a titanium compound which can be thermally hydrolyzed on a continuous strip are described. The layer thus arising is separated from the strip and breaks to form flakes. The flakes thus obtained are alternately coated with a metal oxide hydrate with a high refractive index and a metal oxide hydrate with a low refractive index, by hydrolyzing the corresponding water-soluble metal compounds after or without intermediate drying in a wet process. Again, it is considered disadvantageous that the thus obtained pigments do not show a pronounced colour effect upon rotation. Further at least five layers must be deposited to obtain reasonable colour effects upon tilting resulting in thick pigments.
Diffractive pigments: WO03/011980A1 describes diffractive pigment flakes including single layer or multilayer flakes. The flakes comprise a layer having a reflective surface and a diffractive structure formed on the reflective surface, wherein the pitch and amplitude of the structure are selected to decrease the intensity of a zero order diffracted light beam in order to increase the intensity and colour contrast of higher order diffracted light beam. Methods to manufacture such pigments by vacuum deposition are mentioned. As the colour effect of such pigments is based on first or higher order diffraction only the typical rainbow colour effect of holograms can be realised.
WO04/024836 describes first and higher order diffractive pigments, which separate light into spectral components, similar to a prism, and which include a magnetic layer to selectively align the pigments. This document does not disclose or contemplate zero-order diffractive pigments.
WO03/102084 describes all dielectric optical diffractive pigments, showing first and higher order diffraction.
FR2888491 discloses photoprotective compositions comprising diffractive pigments with a grating period less than or equal to 270nm.
In consequence, there is a need for pigments showing a colour effect upon rotation and/or tilting and for suitable manufacturing processes. Further, there is a need for thinner physical colour pigments compared to state of the art ones. The latter enables the use of more printing and coating techniques for the deposition of lacquers containing the pigments compared to lacquers containing state of the art physical colour pigments.
Thus, it is an object of the present invention to mitigate at least some of these drawbacks of the state of the art. In particular, it is an aim of the present invention to provide new pigments showing a colour effect upon rotation and/or tilting and to provide manufacturing processes for obtaining such pigments. A further aim of this invention is to provide thinner pigments compared to state of the art physical colour pigments.
These objectives are achieved by a matrix comprising a pigment as defined in claim 1 and by a manufacturing process as defined in claim 5. Further aspects of the invention are disclosed in the specification and independent claims, preferred embodiments are disclosed in the specification and the dependent claims.
The present invention will be described in more detail below. It is understood that the various embodiments, preferences and ranges as provided / disclosed in this specification may be combined at will. Further, depending of the specific embodiment, selected definitions, embodiments or ranges may not apply.
Unless otherwise stated, the following definitions shall apply in this specification:

Zero-order diffractive pigments ("ZOD pigments") are pigments showing a colour effect (i.e. change of colour) upon rotation and/or tilting, wherein said colour effect is based on zero-order diffraction.

A material is considered "embossable" if it maintains the structure of an embossing tool on its surface after subjecting it to an embossing step.
A "periodic microstructure" is a periodic structure having a period between 100 nm and 600nm.
The term "pigment" is known in the field. It relates to solid particles, each particle showing a colour and/or a colour effect. Advantageously, said particles have maximum diameters below 100 micrometers (µm), particularly below 20µm. Advantageously, such particles are flake-shaped, i.e. they are thin when compared to its length and width.
The term "high index of refraction layer" ("HRI layer"), is known in the field. For example, the HRI layer can be made of ZnS, TiO₂, Cr₂O₃, AlN, Al₂O₃, HfO₂, Nb₂O₅, Si₃N₄, SnN, Ta₂O₅, V₂O₅, WO₃, or ZrO₂, or similar inorganic materials or high-index polymers like HRI721 and HRI751 (optimate).
The present invention will be better understood by reference to the figures.

Figure 1.1 shows a schematic side view drawing of a known ZOD device. Black denotes HRI material, white low index of refraction material. A is the period and t the depth of the microstructure, p the width of the upper microstructure line, φ the rotational angle, Θ the viewing angle and c the thickness of the HRI layer.
Figure 1.2: Schematic drawing of the top view on a ZOD device describing the colour flip upon rotation about the surface normal for a linear grating. E.g. green light is reflected in a certain viewing angle if the grating lines are perpendicular to the direction of reflection (left part). Rotating the ZOD device by 90° turns the colour from green to red. The grating lines are now in line with the direction of reflection (right part). Other grating symmetries produce other rotational angles.
Figure 1.3a: Alternative ZOD pigment grating shapes: Sinusoidal (above) and triangular (below). Combinations of these two shapes and combinations with rectangular shapes also exhibit zero-order diffraction.
Figure 1.3b: Possible asymmetric ZOD pigment grating shapes: Asymmetric triangular (above) and asymmetric rectangular (below).
Figure 1.4: ZOD pigments (black grating) embedded in paste, liquid, powder or polymer.
Figure 1.5: ZOD pigments (black grating) coated with a polymer, sugar etc to make a small powder particle mixed into other powder particles (light grey).
Figure 2.1 schematically shows a process for manufacturing ZOD pigments as described herein.
Figure 2.2: schematically shows an alternative process for manufacturing ZOD pigments as described herein. It is possible to arrange the first 3 steps in different orders. The geometry of the knife separators during embossing can be different, for example rectangular. Also a depression instead of an enhancement will provide the separator function. However, the height of the knife edge is larger than the full thickness of the dielectric stack.

In more general terms, in a first aspect, the invention relates to a matrix comprising a pigment, in particular zero-order diffraction pigment ("ZOD pigment"), wherein said pigment consists of solid particles, each of said particles having a colour and a colour effect, and each of said particles consisting of an optical waveguiding layer (HRI layer), wherein said layer is made of a material with an index of refraction that is higher than the average index of refraction of the adjacent matrix material by at least 0.25; whereas said layer has a zero-order diffractive resonant grating structure with a period between 100- 600nm (but excluding a period less than or equal to 270nm), and a grating depth between 30-300nm; and whereas said layer has a thickness between 50nm and 500nm.
In an advantageous embodiment, the zero-order diffractive grating structure posses a period that is smaller than the wavelength of the light which shall be reflected in the zeroth reflection order.
In a further advantageous embodiment, the zero-order diffractive grating structure has a grating depth of 150nm or less.
In a further advantageous embodiment, the particles of said pigment have a thickness between 100 nm to 2 micrometer and a lateral size between 1 and 100 micrometer. The shape of such particles can be arbitrary, advantageous shapes are rectangular, triangular, hexagonal, or pentagonal. Although ZOD effects on large area (>2mm²) are known (e.g. US04484797 ), the size effect of ZOD has not been investigated to date. It was surprisingly found that ZOD effects already appear if the grating laterally extends over at least 3 grating periods, as the calculations and experiments involved are difficult. Therefore not only large area ZOD colour effects are possible, but colour pigments based on zero-order diffraction, with a lateral size of at least 1 micrometer can be manufactured. The reflection spectrum of such colour pigments depends besides the above mentioned parameters on the size and shape of the pigment. Without being bound to theory it is believed that for example pigments with a grating period between 300nm and 500nm or less and a lateral size of between 1-2 micrometers have broader reflection peaks than pigments with the same grating but a lateral size of 10 micrometers or more.
In one embodiment of the invention, the following parameters have to be fulfilled: The grating period has to be smaller than the wavelength of the diffracted light. Typical grating periods Λ are in the range between 100 - 600 nm (but excluding a period less than or equal to 270 nm), particularly 300 - 500 nm. Typical grating depths t are between 30 - 300 nm, preferably 150 nm's or less. For dielectric materials, the useful thickness c strongly depends on the grating and the material properties, however, typical thicknesses are in the range of 30nm's - 250nm's.A suitable range for the fill factor f.f.=p/A is 0.3 - 0.8, preferably 0.4 - 0.7. The grating profile also affects the reflection spectrum. Possible grating profiles are rectangular, curved (e.g. sinusoidal), triangular and combinations of these three basic shapes. Advantageous examples of grating shapes are shown in fig. 1.1 and 1.3.
In an advantageous embodiment, the above ZOD pigments consist of particles having an anisotropic lateral shape, in particular an elongated lateral shape. In general, ZOD devices change their colour at different polar angles (theta). This gives ZOD pigments an iridescent appearance when applied to a surface, similar to the colour shifting effects observed with the well established colour shifting interference pigments ( US5135812 ). Further, ZOD devices with linear, one dimensional gratings show a distinct colour flip under 90° rotation about the surface normal. In ZOD pigments, which are deposited with an arbitrary orientation, the colour flip is not observable by the human eye any more. Only the dependence on the polar angle theta will remain. However, if the pigment shape is strongly anisotropic, for example, rectangular and the deposition method favours the alignment of one direction, then the deposited colour pigments will still show a colour flip effect, i.e., the surface will change the colour when it is rotated about the surface normal. Suitable pigments comprise rod-shaped particles, in particular rectangular particles, with a width to length ratio in the range of 1:2 to 1:10, in particular 1:5 (e.g. 10 x 50 micrometers). This can be achieved for example, by depositing long, narrow, rectangular pigments on a surface in a wet coating process with or without a polymeric binder. Printing, especially flexo-printing, ink jet-printing or screen-printing; curtain or dip coating and spraying are suitable techniques. It was found advantageous, if the dried layer has a thickness less than 2 times the longer dimension of the pigment side, resulting in a layer which is at maximum a few micrometers thick.
In a further advantageous embodiment, one or more of the above ZOD pigments are embedded in an organic or inorganic droplet and fixed within this droplet. As shown in fig. 1.5, these droplets are then used as fillers in a powder, paste or gel or also incorporated in liquid or plastic. For pharmaceutical applications or applications in the food industry, the ZOD pigments as described herein might be coated with or embedded in sugars.
In a further embodiment, the invention relates to ZOD pigments consisting of a layer made of a material with an index of refraction that is higher than the index of refraction of the adjacent material whereas the layer has a diffractive grating structure with a period that is smaller than the wavelength of the light which shall be reflected in the zeroth reflection order, preferably between 100-600nm's, but excluding a period less than or equal to 270nm. Typical grating depths are between 30- 300 nm's, preferably 150nm's or less, whereas the layer acts as an optical waveguide and whereas the thickness of the waveguiding layer is between 50nm and 500nm.
In a further advantageous embodiment the invention relates to a matrix, particularly a coating, glaze or lacquer comprising ZOD pigments as described above. A suitable matrix possess an average optical index of refraction at least 0.25 lower than the refractive index of the HRI layer of the ZOD pigment; c.f. fig. 1.4.
In a second aspect, the invention relates to processes, in particular mass production processes, for manufacturing a matrix as described herein wherein for manufacturing said particles said process comprises the steps of i) depositing and optionally micro-structuring on a substrate a first layer which is dissolvable in a first solvent; ii) manufacturing a layer of said pigment by one or more deposition steps and optionally one or more micro-structuring steps wherein all additional layers are insoluble in said first solvent; iii) dissolving said first layer; and v) optionally subjecting the obtained pigments to one or more selection steps as to size and/or shape, wherein at least one micro-structuring step takes place in i) or ii). In the context of this invention, micro-structuring steps are those process steps that produce a micro-structure to one of the manufactured layers; embossing steps are a typical example. In the context of this invention, mass production processes are those processes, that result in large amounts of ZOD pigments; roll-to-roll processes are a typical example.
Similar to the interference layer stack pigments (discussed above), ZOD pigments can be obtained by flaking the high index coatings after micro-structuring and deposition on a flexible web. This can be done by vacuum deposition and embossing methods on large area in roll-to-roll ("R2R") processes. Equipment used for roll-to roll processes is known in the field and may also be used for the manufacturing processes for ZOD pigments as described herein. Thus, in an advantageous embodiment, all steps of the ZOD filter manufacturing process are adapted to fit into such R2R process. Such R2R processes are considered advantageous due to relatively low production costs and high manufacturing speed.
In an embodiment, a first manufacturing process of a ZOD pigment will have the following steps (c.f. fig. 2.2):

1. Hot- or cold embossing of a periodic microstructure ("the grating") into a deformable polymer foil or deformable layer on a polymer foil ("carrier foil"). Suitable materials for the polymer foil ("carrier foil") are thermoplastic polymers. E.g. the carrier foil can be made of acrylonitrile butadiene styrene ABS, polycarbonate PC, polyethylene PE, polyetherimide PEI, polyetherketone PEK, poly(ethylene naphthalate) PEN, poly(ethylene therephtalate) PET, polyimide PI, poly(methyl methacrylate) PMMA, poly-oxy-methylene POM, mono oriented polypropylene MOPP, polystyrene PS, polyvinyl chloride PVC and the like. Suitable materials of the polymeric, deformable layer are poly(vinyl alcohol) PVA, poly(vinyl pyrollidone) PVP and other suitable thermoplastic and coatable polymers. The grating master tool used for embossing, can be metallic, for example a Ni or Steel foil or sheet or plate or roll, with or without Cr surface finish. It might also be made of MoC or WC and the like.
2. Deposition of at least one HRI layer, typically by thermal evaporation, plasma deposition, sputtering or gravure printing. The thickness of each layer is less than 1 micrometer, typically between 50 nm - 500 nm. Thin metal layers might also be deposited by thermal evaporation, plasma deposition or sputtering. The thickness of these layers is typical in the range of 5 nm to 150 nm.
3. The pigments can be peeled off mechanically by dissolving the embossing layer. The pigments can be dissolved in a liquid after the deposition.
4. Pigments can be selected for size and shape, to further narrow down the size distribution. Several sizes can be manufactured at once with this technique.
5. The ZOD- or HRI-pigments are then embedded in paste, powder or distributed in a liquid or paste to be in a processable form.

In an advantageous embodiment, the grating master has small grating patches with borders, which are in the shape of the ZOD pigments. The edges of the gratings are either enhanced or depressed sufficiently, so that each grating on the master is well separated. The intermediate region serves as knife to separate the pigments. As the colour effect of the ZOD pigments can be size dependent, a close control of the pigment shape is needed, for reproducible results and narrow colour spectra. Such size control may be achieved by using a grating master as described herein, as the ZOD pigments shape is controlled at the stage where the grating is manufactured.
In an advantageous embodiment, a release layer is deposited on the embossable foil or layer or on the master tool, preferably on the master tool. This release layer serves as an anti-adhesion layer for the embossing or the HRI layer. Possible examples for release layers are Teflon, DLC, silanes and the like.
The steps and the materials suitable for it are described in further detail below. Reference is also made to figure 2.1, schematically illustrating these steps.
Step a): On a flexible substrate an embossable first layer which can be dissolved in a first solvent is deposited. This can be done for example by roll-to-roll curtain- or cascade coating or gravure printing. The deposition speed with these techniques can be up to several hundreds of meters per minute on flexible web substrates with a web width on the order of one meter. Suitable materials for the flexible substrates are polymer foils for example PET, PEN, PP, PMMA, PS, MOPP, PE, PC and PVC. The thickness of the flexible substrates may be varied in a broad range, but is preferably between 5µm and 500µm, especially preferably between 12µm and 250pm. Such materials are commercially available or obtainable according to known processes. Suitable materials for the first layer are polymers which are embossable and soluble in a solvent, for example Polyester or Nitrocellulose - derivatives. Examples of water soluble and embossable polymers are poly(vinyl pyridine) PVP or poly(vinyl alcohol) PVA. The thickness d₁ of the first layer is typically between 50nm and 10µm, preferred between 100nm and 3µm, especially preferred between 300nm and 2000nm. Suitable solvents for this process step can be chosen according to the selection of material for the first layer. Preferred are environmental friendly solvents. Typically, water, ethanol, isopropanol and its mixtures are used.
Step b1) Next the periodic microstructure is embossed in the first layer. This can be done for example by roll-to-roll hot or cold embossing, wherein the surface of a roll bears the periodic microstructure. Typically this is done by placing a nickel shim around a roll. The periodic micro-structure is as defined above. Pigment shape defining edge knife structures as described in the first method may be used.
Step c1) Next, a second layer which is insoluble in the first solvent and transparent at least in the visible spectral range is deposited on the first layer, wherein transparent means that the average transmission is >75%, preferred > 90%. The thickness d₂ of this second layer must be larger than the depth t of the grating. This ensures to obtain stable flake shaped substrates. Preferred d₂ is in the range of 100 nm up to 2000nm. The deposition can be done by vacuum processes like for example evaporation, sputtering or chemical vapour deposition (CVD). Suitable materials for this second layer are polymers such as poly(p-xylylene) PPX, or inorganic metal oxides or metal halogenides, for example MgF₂, Al₂O₃ or SiO₂. Wet coating techniques like roll-to-roll curtain- or cascade coating or gravure printing are another possibility to deposit the second layer. Examples of materials which can be wet coated and which are insoluble in aqueous solutions are nitrocellulose NC or polystyrene PS. If the second layer is deposited by vacuum deposition the second surface of the second layer, which is not in contact with the first layer, can possess the subwavelength grating structure. This is shown in figure 2.1a). Depending on the material involved and the layer thickness the grating depth and profile may or may not differ on both surfaces. If wet coating techniques are used this second surface will be in most cases uncorrelated with the first surface (not shown in figure 2.1a).
Step d1): Next, the second layer is separated from the flexible substrate by contacting the first layer with a first solvent. Such contact may result in a partial or complete solution of the first layer. The second layer breaks into flakes during the dissolving step.
In an advantageous embodiment, the step d1) can be done in a roll-to-roll process.
In an advantageous embodiment, step d1) may be supported by ultrasonic treatment (US).
Step b2): A second layer, which is embossable and which is insoluble in the above identified first solvent, is deposited on the above identified first layer. Preferred d₂ is in the range of 100 nm up to 2000nm. The same deposition techniques as for the first layer can be used. The second layer can be deposited from micro spheres containing aqueous dispersion. Possible materials are for example Latex or PS micro spheres.
Step c2): Next, the embossing of the periodic microstructure in the second layer takes place. This can be done as described in connection with b1, e.g. by roll-to-roll hot embossing. If the second layer is made of polymeric micro spheres the hot embossing, which is done preferred above the glass transition temperature of the polymeric material, leads to a melting or sealing of the layer. Thus after the hot embossing such a layer is insoluble in water although it was deposited from aqueous solution. Depending on the elastic and plastic properties of the material of the first and the second layer the periodic microstructure is embossed in the upper surface of the second layer or in both surfaces.
Step d2) The second layer is separated from the flexible substrate and forms the flake shaped substrates as described above (d1).
In an advantageous embodiment of this third process the deposition of said first and said second layer takes place simultaneously, e.g. by curtain- or cascade coating.
In an advantageous embodiment of both processes the size and shape of the flakes can be influenced by manufacturing (e.g. embossing) predetermined breaking points or ~lines into the first or the second or in both layers. These breaking points can be for example parallel lines in x- and y-direction. Preferred the thickness of the lines is thin, which means smaller than 3µm, especially smaller than 1.5µm. The spacing between the lines is preferred between 1µm and 100µm, especially preferred between 2µm and 20µm. It was found that an asymmetric shape of the pigments helps to align pigments during the pigment coating process. Such alignment is needed to realise a colour effect upon rotation on products coated with such ZOD pigments. Such breaking points / lines may be manufactured prior, after or simultaneously with embossing of the ZOD microstructure. In a preferred embodiment, the breaking points are embossed together with the periodic microstructure. In this embodiment, the embossing tool comprises the ZOD microstructure and the structure of the ZOD pigments. Thus, no additional equipment is needed.
In many applications pigments are embedded in a polymer matrix with an index of refraction on the order of 1.5 at a wavelength of 550nm. For such applications, the waveguiding layer must be made of a material with an index of refraction at least > 1.75.
In a third aspect, the invention relates to the use of a matrix, as described herein and to a paint, coating, glaze or ink containing a matrix as described herein. Preferably, such matrix can be used in fields like identification, authentication and security, branding and marketing as well as decoration, paints, coatings and cosmetic and pharmaceutical formulations.
Examples of applications are security devices in banknotes, credit cards, passports or for anti-counterfeiting and brand protection. Other possible applications are paints or coatings for automotive or packaging.
ZOD pigments, in particular when embedded in a paste, liquid, powder or polymer may be used in pharmaceutical formulations (e.g. tablets), food, colour coating for cars, plastics, metals, paper and the like.
ZOD pigments coated with a polymer, sugar etc. to make a small powder particle mixed into other powder particles, are useful in pharmaceutical tablets, food or sun cream and the like
To further illustrate the invention, the following examples are provided. These examples are provided with no intend to limit the scope of the invention.

ex.1: On a PET foil (23 micrometer thick) a water soluble PVA layer (1000 nm thick) is applied by gravure printing. Next, a ZOD microstructure is embossed in this PVA layer with a R2R Ni-shim at 100°C. Next, ZnS layer (190 nm thick) is deposited in an evaporation chamber. Pigments are obtained from the coated foil by dissolving the PVA layer in water at room temperature, whereby the hard ZnS layer brittles into small particles of some micrometer in diameter. The size of these particles may be further reduced by US treatment; the size distribution may be reduced by centrifugation or sieving. The obtained pigments show a pronounced colour effect.
ex. 2: The procedure of ex. 1 is followed, with the exception that the Ni-shim also applies predetermined braking lines of 10 * 50 micrometers. The obtained pigments show a pronounced colour effect, no US treatment or steps to amend the size distribution are needed.

Claims

Matrix comprising a pigment, wherein said pigment consists of solid particles, each of said particles having a color and a color effect, and each of said particles consisting of an optical wave-guiding layer, wherein said layer
■ is made of a material with an index of refraction that is higher than the average index of refraction of the adjacent matrix material by at least 0.25,

■ has a zero-order diffractive resonant grating structure with a period between 100-600nm, but excluding a period less than or equal to 270 nm, and a grating depth between 30-300nm and

■ has a thickness between 50nm and 500nm.
Matrix according to claim 1 wherein the zero-order diffractive grating structure possesses a period that is smaller than the wavelength of the light which shall be reflected in the zeroth reflection order.
Matrix according to any of the preceding claims comprising rod-shaped particles having an anisotropic lateral shape with a width to length ratio in the range of 1:2 to 1:10.
Matrix according to any of the preceding claims, wherein said grating structure has a fill factor f.f.=p/A in the range of 0.3 - 0.8.
Process, in particular a roll-to-roll process, for manufacturing a matrix according to any of claims 1 - 6, wherein for manufacturing said particles said process comprises the steps of
■ depositing and optionally micro-structuring on a substrate a first layer which is dissolvable in a first solvent;

■ manufacturing a layer of said pigments by one or more deposition steps and optionally one or more micro-structuring steps;

■ dissolving said first layer for obtaining substrates or pigments;

■ optionally subjecting the obtained substrates or pigments to one or more selection steps as to size and/or shape
wherein at least one micro-structuring step takes place.
Process according to claim 5, wherein the first layer essentially consists of PVA or PVP.
Process according to any of claims 5 or 6, wherein the first solvent essentially consists of water.
Use of the matrix according to any of claims 1 to 4 in the fields of identification, authentication and security, branding, marketing, decoration, cosmetic formulations, pharmaceutical formulations.
Paint, coating, glaze or ink containing a matrix according to any of claims 1 to 4.